Coil topologies for inductive power transfer

ABSTRACT

This disclosure provides systems, methods and apparatus including a magnetic flux device configured to transmit or receive magnetic flux to or from a space beyond the magnetic flux device. In certain configurations, the magnetic flux device can include a first coil with a first layer and second layer, a second coil with a third layer and fourth layer, and a magnetically permeable material with the first coil extending over a first edge of the magnetically permeable material and the second coil extending over a second edge of the magnetically permeable material. In certain other configurations, the magnetic flux device can include a first conductive structure including a first coil and a second coil enclosing a first area and a second area, respectively. The magnetic flux device can further include a second conductive structure with at least a first planar portion of the first conductive structure being substantially coplanar with a second planar portion of the second conductive structure.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of U.S. application Ser. No.14/461,243, filed Aug. 15, 2014, which claims the benefit of priority toU.S. Provisional Appl. No. 61/917,280, filed Dec. 17, 2013. Each ofthese applications is incorporated in its entirety by reference herein.

FIELD

The present disclosure relates generally to wireless power transfer, andmore specifically to devices, systems, and methods related to wirelesspower transfer to remote systems such as electric vehicles, and couplercoil topologies.

BACKGROUND

Remote systems, such as vehicles, have been introduced that includelocomotion power derived from electricity received from an energystorage device such as a battery. For example, hybrid electric vehiclesinclude on-board chargers that use power from vehicle braking andtraditional motors to charge the vehicles. Vehicles that are solelyelectric generally receive the electricity for charging the batteriesfrom other sources. Battery electric vehicles (electric vehicles) areoften proposed to be charged through some type of wired alternatingcurrent (AC) such as household or commercial AC supply sources. Thewired charging connections require cables or other similar connectorsthat are physically connected to a power supply. Cables and similarconnectors may sometimes be inconvenient or cumbersome and have otherdrawbacks. Wireless charging systems that are capable of transferringpower in free space (e.g., via a wireless field) to be used to chargeelectric vehicles may overcome some of the deficiencies of wiredcharging solutions. As such, wireless charging systems and methods thatefficiently and safely transfer power for charging electric vehicles.

SUMMARY

Various implementations of systems, methods and devices within the scopeof the appended claims each have several aspects, no single one of whichis solely responsible for the desirable attributes described herein.Without limiting the scope of the appended claims, some prominentfeatures are described herein.

Details of one or more implementations of the subject matter describedin this specification are set forth in the accompanying drawings and thedescription below. Other features, aspects, and advantages will becomeapparent from the description, the drawings, and the claims. Note thatthe relative dimensions of the following figures may not be drawn toscale.

One aspect of the disclosure provides a magnetic flux device configuredto transmit or receive magnetic flux to or from a space beyond themagnetic flux device. The magnetic flux device comprises at least afirst electrically conductive coil and a second electrically conductivecoil. The first coil has a first layer and second layer. The second coilhas a third layer and fourth layer. The first layer is substantiallycoplanar with the third layer. The magnetic flux device furthercomprises a magnetically permeable material having a substantiallyplanar first surface, a second surface adjoined to the first surface ata first edge, and a third surface adjoined to the first surface at asecond edge. The first coil extends over the first edge and intersects aplane of the first surface. The second coil extends over the second edgeand intersects the plane of the first surface.

Another aspect of the disclosure provides a magnetic flux device forwirelessly receiving or transmitting power from or to a space beyond themagnetic flux device. The magnetic flux device comprises a firstconductive structure configured to wirelessly receive or transmit powervia a magnetic field. The first conductive structure comprises a firstcoil having a first lower surface and a second coil having a secondlower surface, the first lower surface substantially coplanar with thesecond lower surface. The first conductive structure has a first lengthand a first width both substantially parallel to the first and secondlower surfaces, with the first length greater than the first width. Themagnetic flux device further comprises a second conductive structureconfigured to wirelessly receive or transmit power via the magneticfield. The second conductive structure has a second length and a secondwidth both substantially parallel to the first and second lowersurfaces. The second length is substantially parallel to the firstlength and is greater than the second width. At least a first planarportion of the first conductive structure is substantially coplanar witha second planar portion of the second conductive structure.

Another aspect of the disclosure provides a magnetic flux deviceconfigured to transmit or receive magnetic flux to or from a spacebeyond the magnetic flux device. The magnetic flux device comprises atleast a first electrically conductive coil and a second electricallyconductive coil. The first coil is substantially planar and has a firstperiphery bounding a first area. The second coil is substantially planarand has a second periphery bounding a second area. The second coil issubstantially coplanar with the first coil. The magnetic flux devicefurther comprises a magnetically permeable material having asubstantially planar surface and having a third periphery bounding athird area. The first coil and the second coil are substantiallyparallel to the substantially planar surface. A ratio of a sum of thefirst area and the second area to the third area is in a range between0.9 and 1.1.

Another aspect of the disclosure provides a method for transmitting orreceiving magnetic flux. The method comprises flowing at least oneelectric current using at least a first electrically conductive coil anda second electrically conductive coil. The first coil has a first layerand second layer. The second coil has a third layer and fourth layer.The first layer is substantially coplanar with the third layer. Themethod further comprises modifying magnetic flux generated by the atleast one electric current or which generates the at least one electriccurrent. The magnetic flux is modified using a magnetically permeablematerial having a substantially planar first surface, a second surfaceadjoined to the first surface at a first edge, and a third surfaceadjoined to the first surface at a second edge. The first coil extendsover the first edge and intersects a plane of the first surface. Thesecond coil extends over the second edge and intersects the plane of thefirst surface.

Another aspect of the disclosure provides a magnetic flux deviceconfigured to transmit or receive magnetic flux to or from a spacebeyond the magnetic flux device. The magnetic flux device comprisesmeans for flowing at least one electric current and means for modifyingmagnetic flux generated by the at least one electric current or whichgenerates the at least one electric current. The flowing means cancomprise at least a first electrically conductive coil and a secondelectrically conductive coil. The first coil has a first layer andsecond layer. The second coil has a third layer and fourth layer. Thefirst layer is substantially coplanar with the third layer. Themodifying means can comprise a magnetically permeable material having asubstantially planar first surface, a second surface adjoined to thefirst surface at a first edge, and a third surface adjoined to the firstsurface at a second edge. The first coil extends over the first edge andintersects a plane of the first surface. The second coil extends overthe second edge and intersects the plane of the first surface.

Another aspect of the disclosure provides a method for transmitting orreceiving magnetic flux. The method comprises flowing at least one firstelectric current using at least a first conductive structure configuredto wirelessly receive or transmit power via a magnetic field. The firstconductive structure comprises a first coil having a first lower surfaceand a second coil having a second lower surface, the first lower surfacesubstantially coplanar with the second lower surface. The firstconductive structure has a first length and a first width bothsubstantially parallel to the first and second lower surfaces, with thefirst length greater than the first width. The method further comprisesflowing at least one second electric current using at least a secondconductive structure configured to wirelessly receive or transmit powervia the magnetic field. The second conductive structure has a secondlength and a second width both substantially parallel to the first andsecond lower surfaces. The second length is substantially parallel tothe first length and is greater than the second width. At least a firstplanar portion of the first conductive structure is substantiallycoplanar with a second planar portion of the second conductivestructure.

Another aspect of the disclosure provides a magnetic flux device forwirelessly receiving or transmitting power from or to a space beyond themagnetic flux device. The magnetic flux device comprises first means forflowing at least one first electric current. The first flowing means cancomprise a first conductive structure configured to wirelessly receiveor transmit power via a magnetic field. The first conductive structurecomprises a first coil having a first lower surface and a second coilhaving a second lower surface, the first lower surface substantiallycoplanar with the second lower surface. The first conductive structurehas a first length and a first width both substantially parallel to thefirst and second lower surfaces, with the first length greater than thefirst width. The magnetic flux device further comprises second means forflowing at least one second electric current. The second flowing meanscan comprise a second conductive structure configured to wirelesslyreceive or transmit power via the magnetic field. The second conductivestructure has a second length and a second width both substantiallyparallel to the first and second lower surfaces. The second length issubstantially parallel to the first length and is greater than thesecond width. At least a first planar portion of the first conductivestructure is substantially coplanar with a second planar portion of thesecond conductive structure.

Another aspect of the disclosure provides a method for transmitting orreceiving magnetic flux. The method comprises flowing at least oneelectric current using at least a first electrically conductive coil anda second electrically conductive coil. The first coil is substantiallyplanar and has a first periphery bounding a first area. The second coilis substantially planar and has a second periphery bounding a secondarea. The second coil is substantially coplanar with the first coil. Themethod further comprises modifying magnetic flux generated by the atleast one electric current or which generates the at least one electriccurrent. The magnetic flux is modified using a magnetically permeablematerial having a substantially planar surface and having a thirdperiphery bounding a third area. The first coil and the second coil aresubstantially parallel to the substantially planar surface. A ratio of asum of the first area and the second area to the third area is in arange between 0.9 and 1.1.

Another aspect of the disclosure provides a magnetic flux deviceconfigured to transmit or receive magnetic flux to or from a spacebeyond the magnetic flux device. The magnetic flux device comprisesmeans for flowing at least one electric current. The flowing means cancomprise at least a first electrically conductive coil and a secondelectrically conductive coil. The first coil is substantially planar andhas a first periphery bounding a first area. The second coil issubstantially planar and has a second periphery bounding a second area.The second coil is substantially coplanar with the first coil. Themagnetic flux device further comprises means for modifying the magneticflux generated by the at least one electric current or which generatesthe at least one electric current. The modifying means can comprise amagnetically permeable material having a substantially planar surfaceand having a third periphery bounding a third area. The first coil andthe second coil are substantially parallel to the substantially planarsurface. A ratio of a sum of the first area and the second area to thethird area is in a range between 0.9 and 1.1.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a diagram of an exemplary wireless power transfer system forcharging an electric vehicle, in accordance with an exemplary embodimentof the invention.

FIG. 2 is a schematic diagram of exemplary core components of thewireless power transfer system of FIG. 1.

FIG. 3 is another functional block diagram showing exemplary core andancillary components of the wireless power transfer system of FIG. 1.

FIG. 4 is a functional block diagram showing a replaceable contactlessbattery disposed in an electric vehicle, in accordance with an exemplaryembodiment of the invention.

FIGS. 5A, 5B, 5C, and 5D are diagrams of exemplary configurations forthe placement of an induction coil and ferrite material relative to abattery, in accordance with exemplary embodiments of the invention.

FIG. 6 is a chart of a frequency spectrum showing exemplary frequenciesthat may be available for wireless charging an electric vehicle, inaccordance with an exemplary embodiment of the invention.

FIG. 7 is a chart showing exemplary frequencies and transmissiondistances that may be useful in wireless charging electric vehicles, inaccordance with an exemplary embodiment of the invention.

FIG. 8A shows a family of “double-coil”-type inductive power transfer(IPT) coupler designs that may be considered as having been generated bya process of metamorphosis of a “circular”-type coupler towards a“solenoid”-type coupler.

FIG. 8B schematically illustrates a process of metamorphosis from a“circular”-type coupler towards a “solenoid”-type coupler.

FIG. 9A schematically illustrates the cross-section of a so-called“circular”-type coupler comprising a “circular”-type coil structure, aferrite structure, and a conductive back plate, as well as the typicaldirections of currents and lines of magnetic field for this coiltopology.

FIG. 9B shows a perspective view of a “circular”-type coupler model inaccordance with FIG. 9A with a rectangular-shaped coil having roundedcorners (e.g., an ‘O’-shaped coil).

FIG. 10 schematically illustrates the cross-section of an IPT coupler inaccordance with FIG. 9A with the coil split into two halves (e.g., coilA and coil B).

FIG. 11 schematically illustrates coil A moved to the left.

FIG. 12 schematically illustrates coil B moved to the right.

FIG. 13A schematically illustrates coil A lowered to the same plane ascoil B, as well as the current directions and lines of magnetic fieldfor a mode of operation that generates a ‘vertical’ magnetic moment.

FIG. 13B shows a perspective view of an IPT coupler model in accordancewith FIG. 13A, and more specifically, a so-called “bipolar”-type couplerthat is characterized by two overlapping coils with coil A and coil Bhaving substantially ‘zero’ mutual inductance.

FIG. 14 schematically illustrates the cross-section of an IPT couplertopology in accordance with FIG. 13A but with the current direction ofcoil B reversed so that the magnetic flux device generates a‘horizontal’ magnetic moment, indicated by two distinct magnetic poleareas (N) and (S) and a field line starting at one pole area and endingat the other pole area.

FIG. 15A schematically illustrates coil A and coil B further separatedand somewhat contracted so that they do not overlap, as well as thecurrent directions and a field line indicating a mode of operation thatgenerates a horizontal magnetic moment.

FIG. 15B shows a perspective view of an IPT coupler model in accordancewith FIG. 15A, and more specifically a so-called “double-D”-typemagnetic flux device that is characterized by two non-overlapping coilshaving some mutual inductance and by a ferrite backing havingessentially the same size as the “double-D”-type coil structure, termedthe “double-D—full size ferrite” coupler topology.

FIG. 16A schematically illustrates the cross-section of an IPT couplersimilar to FIG. 15A but with a length and width of the ferrite backingmade smaller so that the outer parts of the “double-D”-type coils areoverhanging the ferrite backing.

FIG. 16B shows a perspective view of an IPT coupler model in accordancewith FIG. 16A that is termed the “double-D, planar overhanging windings”coupler topology.

FIG. 17A schematically illustrates the outer segments of the“double-D”-type coil further moved out and folded so that windings atboth front sides are stacked with windings below the plane of thesurface of the ferrite backing and closer to the back plate.

FIG. 17B shows a perspective view of an IPT coupler model in accordancewith FIG. 17A that is termed the “double-D, front stacked windings”coupler topology.

FIG. 18 schematically illustrates the coils of the “double-D, frontstacked windings” coupler topology on opposite side of the ferritestructure and the air gap between ferrite and back plate increased,which is termed the “double solenoid, front stacked windings” couplertopology.

FIG. 19 schematically illustrates the bottom segments of the coilsunfolded to a single layer winding and slightly moved towards the centerof the magnetic flux device, which may be considered as two obliquesolenoid coils and is termed the “double solenoid, oblique windings”coupler topology.

FIG. 20 schematically illustrates the cross-section of the IPT couplertopology of FIG. 19 but with the length of the ferrite increased tomatch the size of the coil structure, which is termed the “doublesolenoid, oblique windings, full size ferrite” coupler topology.

FIG. 21 schematically illustrates the two oblique solenoid coils furthercontracted and moved towards the center, which is termed the “doublesolenoid, slightly oblique windings” coupler topology.

FIG. 22 schematically illustrates the cross-section of an IPT couplertopology using two solenoid coils directly adjacent with currents in thesame direction, which is termed the “double solenoid, adjacent windings”coupler topology.

FIG. 23A schematically illustrates the cross-section of an IPT couplerwith the two coils merged into a single coil, which may be considered asthe planar “solenoid”-type magnetic flux device.

FIG. 23B shows a perspective view of the planar “solenoid”-type couplermodel in accordance with FIG. 23A.

FIG. 24 schematically illustrates an overview of all the steps ofmetamorphosis as depicted in the previous figures with step numbersindicated.

FIG. 25 shows a perspective view of a model of a variant of the“double-D”-type coupler with the coil size (overall length and widthform factor) substantially the same as the size of the ferritestructure, which is termed the “double-D, full size ferrite” coupler.

FIGS. 26A-26C shows a transparent top-down view, a perspective cut view,and an explosion view, respectively, of a model of the “double-D, frontstacked windings” magnetic flux device.

FIG. 26D shows a potential space for electronics in a small vehiclepackage integrated solution using a “double-D, front stacked winding”magnetic flux device.

FIGS. 27A-27C shows a transparent top down view, a perspective cut view,and an explosion view, respectively, of a model of a “cross-polar”-typecoupler (“DDQ” coupler) that integrates both a “double-D” coil and a“circular” (‘Q’) coil.

The various features illustrated in the drawings may not be drawn toscale. Accordingly, the dimensions of the various features may bearbitrarily expanded or reduced for clarity. In addition, some of thedrawings may not depict all of the components of a given system, methodor device. Finally, like reference numerals may be used to denote likefeatures throughout the specification and figures.

DETAILED DESCRIPTION

The detailed description set forth below in connection with the appendeddrawings is intended as a description of exemplary embodiments of theinvention and is not intended to represent the only embodiments in whichthe invention may be practiced. The term “exemplary” used throughoutthis description means “serving as an example, instance, orillustration,” and should not necessarily be construed as preferred oradvantageous over other exemplary embodiments. The detailed descriptionincludes specific details for the purpose of providing a thoroughunderstanding of the exemplary embodiments of the invention. In someinstances, some devices are shown in block diagram form.

Wirelessly transferring power may refer to transferring any form ofenergy associated with electric fields, magnetic fields, electromagneticfields, or otherwise from a transmitter to a receiver without the use ofphysical electrical conductors (e.g., power may be transferred throughfree space). The power output into a wireless field (e.g., a magneticfield) may be received, captured by, or coupled by a “receiving coil” toachieve power transfer.

An electric vehicle is used herein to describe a remote system, anexample of which is a vehicle that includes, as part of its locomotioncapabilities, electrical power derived from a chargeable energy storagedevice (e.g., one or more rechargeable electrochemical cells or othertype of battery). As non-limiting examples, some electric vehicles maybe hybrid electric vehicles that include besides electric motors, atraditional combustion engine for direct locomotion or to charge thevehicle's battery. Other electric vehicles may draw all locomotionability from electrical power. An electric vehicle is not limited to anautomobile and may include motorcycles, carts, scooters, and the like.By way of example and not limitation, a remote system is describedherein in the form of an electric vehicle (EV). Furthermore, otherremote systems that may be at least partially powered using a chargeableenergy storage device are also contemplated (e.g., electronic devicessuch as personal computing devices and the like).

FIG. 1 is a diagram of an exemplary wireless power transfer system 100for charging an electric vehicle 112, in accordance with an exemplaryembodiment of the invention. The wireless power transfer system 100enables charging of an electric vehicle 112 while the electric vehicle112 is parked near a base wireless charging system 102 a. Spaces for twoelectric vehicles are illustrated in a parking area to be parked overcorresponding base wireless charging system 102 a and 102 b. In someembodiments, a local distribution center 130 may be connected to a powerbackbone 132 and configured to provide an alternating current (AC) or adirect current (DC) supply through a power link 110 to the base wirelesscharging system 102 a. The base wireless charging system 102 a alsoincludes a base system induction coil 104 a for wirelessly transferringor receiving power. An electric vehicle 112 may include a battery unit118, an electric vehicle induction coil 116, and an electric vehiclewireless charging system 114. The electric vehicle induction coil 116may interact with the base system induction coil 104 a for example, viaa region of the electromagnetic field generated by the base systeminduction coil 104 a.

In some exemplary embodiments, the electric vehicle induction coil 116may receive power when the electric vehicle induction coil 116 islocated in an energy field produced by the base system induction coil104 a. The field corresponds to a region where energy output by the basesystem induction coil 104 a may be captured by an electric vehicleinduction coil 116. For example, the energy output by the base systeminduction coil 104 a may be at a level sufficient to charge or power theelectric vehicle 112. In some cases, the field may correspond to the“near field” of the base system induction coil 104 a. The near-field maycorrespond to a region in which there are strong reactive fieldsresulting from the currents and charges in the base system inductioncoil 104 a that do not radiate power away from the base system inductioncoil 104 a. In some cases the near-field may correspond to a region thatis within about ½π of wavelength of the base system induction coil 104 a(and vice versa for the electric vehicle induction coil 116) as will befurther described below.

Local distribution 1130 may be configured to communicate with externalsources (e.g., a power grid) via a communication backhaul 134, and withthe base wireless charging system 102 a via a communication link 108.

In some embodiments the electric vehicle induction coil 116 may bealigned with the base system induction coil 104 a and, therefore,disposed within a near-field region simply by the driver positioning theelectric vehicle 112 correctly relative to the base system inductioncoil 104 a. In other embodiments, the driver may be given visualfeedback, auditory feedback, or combinations thereof to determine whenthe electric vehicle 112 is properly placed for wireless power transfer.In yet other embodiments, the electric vehicle 112 may be positioned byan autopilot system, which may move the electric vehicle 112 back andforth (e.g., in zig-zag movements) until an alignment error has reacheda tolerable value. This may be performed automatically and autonomouslyby the electric vehicle 112 without or with only minimal driverintervention provided that the electric vehicle 112 is equipped with aservo steering wheel, ultrasonic sensors, and intelligence to adjust thevehicle. In still other embodiments, the electric vehicle induction coil116, the base system induction coil 104 a, or a combination thereof mayhave functionality for displacing and moving the induction coils 116 and104 a relative to each other to more accurately orient them and developmore efficient coupling therebetween.

The base wireless charging system 102 a may be located in a variety oflocations. As non-limiting examples, some suitable locations include aparking area at a home of the electric vehicle 112 owner, parking areasreserved for electric vehicle wireless charging modeled afterconventional petroleum-based filling stations, and parking lots at otherlocations such as shopping centers and places of employment.

Charging electric vehicles wirelessly may provide numerous benefits. Forexample, charging may be performed automatically, virtually withoutdriver intervention and manipulations thereby improving convenience to auser. There may also be no exposed electrical contacts and no mechanicalwear out, thereby improving reliability of the wireless power transfersystem 100. Manipulations with cables and connectors may not be needed,and there may be no cables, plugs, or sockets that may be exposed tomoisture and water in an outdoor environment, thereby improving safety.There may also be no sockets, cables, and plugs visible or accessible,thereby reducing potential vandalism of power charging devices. Further,since an electric vehicle 112 may be used as distributed storage devicesto stabilize a power grid, a docking-to-grid solution may be used toincrease availability of vehicles for Vehicle-to-Grid (V2G) operation.

A wireless power transfer system 100 as described with reference to FIG.1 may also provide aesthetical and non-impedimental advantages. Forexample, there may be no charge columns and cables that may beimpedimental for vehicles and/or pedestrians.

As a further explanation of the vehicle-to-grid capability, the wirelesspower transmit and receive capabilities may be configured to bereciprocal such that the base wireless charging system 102 a transferspower to the electric vehicle 112 and the electric vehicle 112 transferspower to the base wireless charging system 102 a e.g., in times ofenergy shortfall. This capability may be useful to stabilize the powerdistribution grid by allowing electric vehicles to contribute power tothe overall distribution system in times of energy shortfall caused byover demand or shortfall in renewable energy production (e.g., wind orsolar).

FIG. 2 is a schematic diagram of exemplary core components of thewireless power transfer system 100 of FIG. 1. As shown in FIG. 2, thewireless power transfer system 200 may include a base system transmitcircuit 206 including a base system induction coil 204 having aninductance L₁. The wireless power transfer system 200 further includesan electric vehicle receive circuit 222 including an electric vehicleinduction coil 216 having an inductance L₂. Embodiments described hereinmay use capacitively loaded wire loops (i.e., multi-turn coils) forminga resonant structure that is capable of efficiently coupling energy froma primary structure (transmitter) to a secondary structure (receiver)via a magnetic or electromagnetic near field if both primary andsecondary are tuned to a common resonant frequency. The coils may beused for the electric vehicle induction coil 216 and the base systeminduction coil 204. Using resonant structures for coupling energy may bereferred to “magnetic coupled resonance,” “electromagnetic coupledresonance,” and/or “resonant induction.” The operation of the wirelesspower transfer system 200 will be described based on power transfer froma base wireless power charging system 202 to an electric vehicle 112,but is not limited thereto. For example, as discussed above, theelectric vehicle 112 may transfer power to the base wireless chargingsystem 102 a.

With reference to FIG. 2, a power supply 208 (e.g., AC or DC) suppliespower P_(SDC) to the base wireless power charging system 202 to transferenergy to an electric vehicle 112. The base wireless power chargingsystem 202 includes a base charging system power converter 236. The basecharging system power converter 236 may include circuitry such as anAC/DC converter configured to convert power from standard mains AC to DCpower at a suitable voltage level, and a DC/low frequency (LF) converterconfigured to convert DC power to power at an operating frequencysuitable for wireless high power transfer. The base charging systempower converter 236 supplies power P₁ to the base system transmitcircuit 206 including the capacitor C₁ in series with the base systeminduction coil 204 to emit an electromagnetic field at a desiredfrequency. The capacitor C₁ may be provided to form a resonant circuitwith the base system induction coil 204 that resonates at a desiredfrequency. The base system induction coil 204 receives the power P₁ andwirelessly transmits power at a level sufficient to charge or power theelectric vehicle 112. For example, the power level provided wirelesslyby the base system induction coil 204 may be on the order of kilowatts(kW) (e.g., anywhere from 1 kW to 110 kW or higher or lower).

The base system transmit circuit 206 including the base system inductioncoil 204 and electric vehicle receive circuit 222 including the electricvehicle induction coil 216 may be tuned to substantially the samefrequencies and may be positioned within the near-field of anelectromagnetic field transmitted by one of the base system inductioncoil 204 and the electric vehicle induction coil 116. In this case, thebase system induction coil 204 and electric vehicle induction coil 116may become coupled to one another such that power may be transferred tothe electric vehicle receive circuit 222 including capacitor C₂ andelectric vehicle induction coil 116. The capacitor C₂ may be provided toform a resonant circuit with the electric vehicle induction coil 216that resonates at a desired frequency. Element k(d) represents themutual coupling coefficient resulting at coil separation. Equivalentresistances R_(eq,1) and R_(eq,2) represent the losses that may beinherent to the induction coils 204 and 216 and the anti-reactancecapacitors C₁ and C₂. The electric vehicle receive circuit 222 includingthe electric vehicle induction coil 316 and capacitor C₂ receives powerP₂ and provides the power P₂ to an electric vehicle power converter 238of an electric vehicle charging system 214.

The electric vehicle power converter 238 may include, among otherthings, a LF/DC converter configured to convert power at an operatingfrequency back to DC power at a voltage level matched to the voltagelevel of an electric vehicle battery unit 218. The electric vehiclepower converter 238 may provide the converted power P_(LDC) to chargethe electric vehicle battery unit 218. The power supply 208, basecharging system power converter 236, and base system induction coil 204may be stationary and located at a variety of locations as discussedabove. The battery unit 218, electric vehicle power converter 238, andelectric vehicle induction coil 216 may be included in an electricvehicle charging system 214 that is part of electric vehicle 112 or partof the battery pack (not shown). The electric vehicle charging system214 may also be configured to provide power wirelessly through theelectric vehicle induction coil 216 to the base wireless power chargingsystem 202 to feed power back to the grid. Each of the electric vehicleinduction coil 216 and the base system induction coil 204 may act astransmit or receive induction coils based on the mode of operation.

While not shown, the wireless power transfer system 200 may include aload disconnect unit (LDU) to safely disconnect the electric vehiclebattery unit 218 or the power supply 208 from the wireless powertransfer system 200. For example, in case of an emergency or systemfailure, the LDU may be triggered to disconnect the load from thewireless power transfer system 200. The LDU may be provided in additionto a battery management system for managing charging to a battery, or itmay be part of the battery management system.

Further, the electric vehicle charging system 214 may include switchingcircuitry (not shown) for selectively connecting and disconnecting theelectric vehicle induction coil 216 to the electric vehicle powerconverter 238. Disconnecting the electric vehicle induction coil 216 maysuspend charging and also may adjust the “load” as “seen” by the basewireless charging system 102 a (acting as a transmitter), which may beused to “cloak” the electric vehicle charging system 114 (acting as thereceiver) from the base wireless charging system 102 a. The load changesmay be detected if the transmitter includes the load sensing circuit.Accordingly, the transmitter, such as a base wireless charging system202, may have a mechanism for determining when receivers, such as anelectric vehicle charging system 114, are present in the near-field ofthe base system induction coil 204.

As described above, in operation, assuming energy transfer towards thevehicle or battery, input power is provided from the power supply 208such that the base system induction coil 204 generates a field forproviding the energy transfer. The electric vehicle induction coil 216couples to the radiated field and generates output power for storage orconsumption by the electric vehicle 112. As described above, in someembodiments, the base system induction coil 204 and electric vehicleinduction coil 116 are configured according to a mutual resonantrelationship such that when the resonant frequency of the electricvehicle induction coil 116 and the resonant frequency of the base systeminduction coil 204 are very close or substantially the same.Transmission losses between the base wireless power charging system 202and electric vehicle charging system 214 are minimal when the electricvehicle induction coil 216 is located in the near-field of the basesystem induction coil 204.

As stated, an efficient energy transfer occurs by coupling a largeportion of the energy in the near field of a transmitting induction coilto a receiving induction coil rather than propagating most of the energyin an electromagnetic wave to the far-field. When in the near field, acoupling mode may be established between the transmit induction coil andthe receive induction coil. The area around the induction coils wherethis near field coupling may occur is referred to herein as a near fieldcoupling mode region.

While not shown, the base charging system power converter 236 and theelectric vehicle power converter 238 may both include an oscillator, adriver circuit such as a power amplifier, a filter, and a matchingcircuit for efficient coupling with the wireless power induction coil.The oscillator may be configured to generate a desired frequency, whichmay be adjusted in response to an adjustment signal. The oscillatorsignal may be amplified by a power amplifier with an amplificationamount responsive to control signals. The filter and matching circuitmay be included to filter out harmonics or other unwanted frequenciesand match the impedance of the power conversion module to the wirelesspower induction coil. The power converters 236 and 238 may also includea rectifier and switching circuitry to generate a suitable power outputto charge the battery.

The electric vehicle induction coil 216 and base system induction coil204 as described throughout the disclosed embodiments may be referred toor configured as “loop” antennas, and more specifically, multi-turn loopantennas. The induction coils 204 and 216 may also be referred to hereinor be configured as “magnetic” antennas. The term “coil” generallyrefers to a component that may wirelessly output or receive energy forcoupling to another “coil.” The coil may also be referred to as an“antenna” of a type that is configured to wirelessly output or receivepower. As used herein, coils 204 and 216 are examples of “power transfercomponents” of a type that are configured to wirelessly output,wirelessly receive, and/or wirelessly relay power. Loop (e.g.,multi-turn loop) antennas may be configured to include an air core or aphysical core such as a ferrite core. An air core loop antenna may allowthe placement of other components within the core area. Physical coreantennas including ferromagnetic or ferromagnetic materials may allowdevelopment of a stronger electromagnetic field and improved coupling.

As discussed above, efficient transfer of energy between a transmitterand receiver occurs during matched or nearly matched resonance between atransmitter and a receiver. However, even when resonance between atransmitter and receiver are not matched, energy may be transferred at alower efficiency. Transfer of energy occurs by coupling energy from thenear field of the transmitting induction coil to the receiving inductioncoil residing within a region (e.g., within a predetermined frequencyrange of the resonant frequency, or within a predetermined distance ofthe near-field region) where this near field is established rather thanpropagating the energy from the transmitting induction coil into freespace.

A resonant frequency may be based on the inductance and capacitance of atransmit circuit including an induction coil (e.g., the base systeminduction coil 204) as described above. As shown in FIG. 2, inductancemay generally be the inductance of the induction coil, whereas,capacitance may be added to the induction coil to create a resonantstructure at a desired resonant frequency. As a non-limiting example, asshown in FIG. 2, a capacitor may be added in series with the inductioncoil to create a resonant circuit (e.g., the base system transmitcircuit 206) that generates an electromagnetic field. Accordingly, forlarger diameter induction coils, the value of capacitance needed toinduce resonance may decrease as the diameter or inductance of the coilincreases. Inductance may also depend on a number of turns of aninduction coil. Furthermore, as the diameter of the induction coilincreases, the efficient energy transfer area of the near field mayincrease. Other resonant circuits are possible. As another non limitingexample, a capacitor may be placed in parallel between the two terminalsof the induction coil (e.g., a parallel resonant circuit). Furthermorean induction coil may be designed to have a high native quality (Q)factor to lower the losses of the induction coil and to increaseefficiency of the inductive coupling system. For example, the native Qfactor may be 300 or greater.

As described above, according to some embodiments, coupling powerbetween two induction coils that are in the near field of one another isdisclosed. As described above, the near field may correspond to a regionaround the induction coil in which electromagnetic fields exist but maynot propagate or radiate away from the induction coil. Near-fieldcoupling-mode regions may correspond to a volume that is near thephysical volume of the induction coil, typically within a small fractionof the wavelength. According to some embodiments, electromagneticinduction coils, such as single and multi-turn loop antennas, are usedfor both transmitting and receiving since magnetic near field amplitudesin practical embodiments tend to be higher for magnetic type coils incomparison to the electric near fields of an electric type antenna(e.g., a small dipole). This allows for potentially higher couplingbetween the pair. Furthermore, “electric” antennas (e.g., dipoles andmonopoles) or a combination of magnetic and electric antennas may beused.

FIG. 3 is another functional block diagram showing exemplary core andancillary components of the wireless power transfer system 300 ofFIG. 1. The wireless power transfer system 300 illustrates acommunication link 376, a guidance link 366, and alignment systems 352,354 for the base system induction coil 304 and electric vehicleinduction coil 316. As described above with reference to FIG. 2, andassuming energy flow towards the electric vehicle 112, in FIG. 3 a basecharging system power interface 354 may be configured to provide powerto a charging system power converter 336 from a power source, such as anAC or DC power supply 126. The base charging system power converter 336may receive AC or DC power from the base charging system power interface354 to excite the base system induction coil 304 at or near its resonantfrequency. The electric vehicle induction coil 316, when in the nearfield coupling-mode region, may receive energy from the near fieldcoupling mode region to oscillate at or near the resonant frequency. Theelectric vehicle power converter 338 converts the oscillating signalfrom the electric vehicle induction coil 316 to a power signal suitablefor charging a battery via the electric vehicle power interface.

The base wireless charging system 302 includes a base charging systemcontroller 345 and the electric vehicle charging system 314 includes anelectric vehicle controller 344. The base charging system controller 345may include a base charging system communication interface 162 to othersystems (not shown) such as, for example, a computer, and a powerdistribution center, or a smart power grid. The electric vehiclecontroller 344 may include an electric vehicle communication interfaceto other systems (not shown) such as, for example, an on-board computeron the vehicle, other battery charging controller, other electronicsystems within the vehicles, and remote electronic systems.

The base charging system controller 345 and electric vehicle controller344 may include subsystems or modules for specific application withseparate communication channels. These communications channels may beseparate physical channels or separate logical channels. As non-limitingexamples, a base charging alignment system 352 may communicate with anelectric vehicle alignment system 354 through a communication link 376to provide a feedback mechanism for more closely aligning the basesystem induction coil 304 and electric vehicle induction coil 316,either autonomously or with operator assistance. Similarly, a basecharging guidance system 362 may communicate with an electric vehicleguidance system 364 through a guidance link to provide a feedbackmechanism to guide an operator in aligning the base system inductioncoil 304 and electric vehicle induction coil 316. In addition, there maybe separate general-purpose communication links (e.g., channels)supported by base charging communication system 372 and electric vehiclecommunication system 374 for communicating other information between thebase wireless power charging system 302 and the electric vehiclecharging system 314. This information may include information aboutelectric vehicle characteristics, battery characteristics, chargingstatus, and power capabilities of both the base wireless power chargingsystem 302 and the electric vehicle charging system 314, as well asmaintenance and diagnostic data for the electric vehicle 112. Thesecommunication channels may be separate physical communication channelssuch as, for example, Bluetooth, zigbee, cellular, etc.

Electric vehicle controller 344 may also include a battery managementsystem (BMS) (not shown) that manages charge and discharge of theelectric vehicle principal battery, a parking assistance system based onmicrowave or ultrasonic radar principles, a brake system configured toperform a semi-automatic parking operation, and a steering wheel servosystem configured to assist with a largely automated parking ‘park bywire’ that may provide higher parking accuracy, thus reducing the needfor mechanical horizontal induction coil alignment in any of the basewireless charging system 102 a and the electric vehicle charging system114. Further, electric vehicle controller 344 may be configured tocommunicate with electronics of the electric vehicle 112. For example,electric vehicle controller 344 may be configured to communicate withvisual output devices (e.g., a dashboard display), acoustic/audio outputdevices (e.g., buzzer, speakers), mechanical input devices (e.g.,keyboard, touch screen, and pointing devices such as joystick,trackball, etc.), and audio input devices (e.g., microphone withelectronic voice recognition).

Furthermore, the wireless power transfer system 300 may includedetection and sensor systems. For example, the wireless power transfersystem 300 may include sensors for use with systems to properly guidethe driver or the vehicle to the charging spot, sensors to mutuallyalign the induction coils with the required separation/coupling, sensorsto detect objects that may obstruct the electric vehicle induction coil316 from moving to a particular height and/or position to achievecoupling, and safety sensors for use with systems to perform a reliable,damage free, and safe operation of the system. For example, a safetysensor may include a sensor for detection of presence of animals orchildren approaching the wireless power induction coils 104 a, 116beyond a safety radius, detection of metal objects near the base systeminduction coil 304 that may be heated up (induction heating), detectionof hazardous events such as incandescent objects on the base systeminduction coil 304, and temperature monitoring of the base wirelesspower charging system 302 and electric vehicle charging system 314components.

The wireless power transfer system 300 may also support plug-in chargingvia a wired connection. A wired charge port may integrate the outputs ofthe two different chargers prior to transferring power to or from theelectric vehicle 112. Switching circuits may provide the functionalityas needed to support both wireless charging and charging via a wiredcharge port.

To communicate between a base wireless charging system 302 and anelectric vehicle charging system 314, the wireless power transfer system300 may use both in-band signaling and an RF data modem (e.g., Ethernetover radio in an unlicensed band). The out-of-band communication mayprovide sufficient bandwidth for the allocation of value-add services tothe vehicle user/owner. A low depth amplitude or phase modulation of thewireless power carrier may serve as an in-band signaling system withminimal interference.

In addition, some communication may be performed via the wireless powerlink without using specific communications antennas. For example, thewireless power induction coils 304 and 316 may also be configured to actas wireless communication transmitters. Thus, some embodiments of thebase wireless power charging system 302 may include a controller (notshown) for enabling keying type protocol on the wireless power path. Bykeying the transmit power level (amplitude shift keying) at predefinedintervals with a predefined protocol, the receiver may detect a serialcommunication from the transmitter. The base charging system powerconverter 336 may include a load sensing circuit (not shown) fordetecting the presence or absence of active electric vehicle receiversin the vicinity of the near field generated by the base system inductioncoil 304. By way of example, a load sensing circuit monitors the currentflowing to the power amplifier, which is affected by the presence orabsence of active receivers in the vicinity of the near field generatedby base system induction coil 104 a. Detection of changes to the loadingon the power amplifier may be monitored by the base charging systemcontroller 345 for use in determining whether to enable the oscillatorfor transmitting energy, to communicate with an active receiver, or acombination thereof.

To enable wireless high power transfer, some embodiments may beconfigured to transfer power at a frequency in the range from 10-150 kHzand particularly in the range from 80-90 kHz. This low frequencycoupling may allow highly efficient power conversion that may beachieved using solid state devices. In addition, there may be lesscoexistence issues with radio systems compared to other bands.

The wireless power transfer system 100 described may be used with avariety of electric vehicles 102 including rechargeable or replaceablebatteries. FIG. 4 is a functional block diagram showing a replaceablecontactless battery disposed in an electric vehicle 412, in accordancewith an exemplary embodiment of the invention. In this embodiment, thelow battery position may be useful for an electric vehicle battery unitthat integrates a wireless power interface (e.g., a charger-to-batterycordless interface 496) and that may receive power from a charger (notshown) embedded in the ground. In FIG. 4, the electric vehicle batteryunit may be a rechargeable battery unit, and may be accommodated in abattery compartment 494. The electric vehicle battery unit also providesa wireless power interface 496, which may integrate the entire electricvehicle wireless power subsystem including a resonant induction coil,power conversion circuitry, and other control and communicationsfunctions as needed for efficient and safe wireless energy transferbetween a ground-based wireless charging unit and the electric vehiclebattery unit.

It may be useful for the electric vehicle induction coil to beintegrated flush with a bottom side of electric vehicle battery unit orthe vehicle body so that there are no protrusive parts and so that thespecified ground-to-vehicle body clearance may be maintained. Thisconfiguration may require some room in the electric vehicle battery unitdedicated to the electric vehicle wireless power subsystem. The electricvehicle battery unit 492 may also include a battery-to-EV cordlessinterface 492, and a charger-to-battery cordless interface 496 thatprovides contactless power and communication between the electricvehicle 412 and a base wireless charging system 102 a as shown in FIG.1.

In some embodiments, and with reference to FIG. 1, the base systeminduction coil 104 a and the electric vehicle induction coil 116 may bein a fixed position and the induction coils are brought within anear-field coupling region by overall placement of the electric vehicleinduction coil 116 relative to the base wireless charging system 102 a.However, in order to perform energy transfer rapidly, efficiently, andsafely, the distance between the base system induction coil 104 a andthe electric vehicle induction coil 116 may need to be reduced toimprove coupling. Thus, in some embodiments, the base system inductioncoil 104 a and/or the electric vehicle induction coil 116 may bedeployable and/or moveable to bring them into better alignment.

FIGS. 5A, 5B, 5C, and 5D are diagrams of exemplary configurations forthe placement of an induction coil and ferrite material relative to abattery, in accordance with exemplary embodiments of the invention. FIG.5A shows a fully ferrite embedded induction coil 536 a. The wirelesspower induction coil may include a ferrite material 538 a and a coil 536a wound about the ferrite material 538 a. The coil 536 a itself may bemade of stranded Litz wire. A conductive shield 532 a may be provided toprotect passengers of the vehicle from excessive EMF transmission.Conductive shielding may be particularly useful in vehicles made ofplastic or composites.

FIG. 5B shows an optimally dimensioned ferrite plate (i.e., ferritebacking) to enhance coupling and to reduce eddy currents (heatdissipation) in the conductive shield 532 b. The coil 536 b may be fullyembedded in a non-conducting non-magnetic (e.g., plastic) material. Forexample, as illustrated in FIGS. 5A-5D, the coil 536 b may be embeddedin a protective housing 534 b. There may be a separation between thecoil 536 b and the ferrite material 538 b as the result of a trade-offbetween magnetic coupling and ferrite hysteresis losses.

FIG. 5C illustrates another embodiment where the coil 536 c (e.g., acopper Litz wire multi-turn coil) may be movable in a lateral (“X”)direction. FIG. 5D illustrates another embodiment where the inductioncoil module is deployed in a downward direction. In some embodiments,the battery unit includes one of a deployable and non-deployableelectric vehicle induction coil module 540 d as part of the wirelesspower interface. To prevent magnetic fields from penetrating into thebattery space 530 d and into the interior of the vehicle, there may be aconductive shield 532 d (e.g., a copper sheet) between the battery space530 d and the vehicle. Furthermore, a non-conductive (e.g., plastic)protective layer 533 d may be used to protect the conductive shield 532d, the coil 536 d, and the ferrite material 538 d from environmentalimpacts (e.g., mechanical damage, oxidization, etc.). Furthermore, thecoil 536 d may be movable in lateral X and/or Y directions. FIG. 5Dillustrates an embodiment wherein the electric vehicle induction coilmodule 540 d is deployed in a downward Z direction relative to a batteryunit body.

The design of this deployable electric vehicle induction coil module 542b is similar to that of FIG. 5B except there is no conductive shieldingat the electric vehicle induction coil module 542 d. The conductiveshield 532 d stays with the battery unit body. The protective layer 533d (e.g., plastic layer) is provided between the conductive shield 432 dand the electric vehicle induction coil module 542 d when the electricvehicle induction coil module 542 d is not in a deployed state. Thephysical separation of the electric vehicle induction coil module 542from the battery unit body may have a positive effect on the inductioncoil's performance.

As discussed above, the electric vehicle induction coil module 542 dthat is deployed may contain only the coil 536 d (e.g., Litz wire) andferrite material 538 d. Ferrite backing may be provided to enhancecoupling and to prevent from excessive eddy current losses in avehicle's underbody or in the conductive shield 532 d. Moreover, theelectric vehicle induction coil module 542 d may include a flexible wireconnection to power conversion electronics and sensor electronics. Thiswire bundle may be integrated into the mechanical gear for deploying theelectric vehicle induction coil module 542 d.

With reference to FIG. 1, the charging systems described above may beused in a variety of locations for charging an electric vehicle 112, ortransferring power back to a power grid. For example, the transfer ofpower may occur in a parking lot environment. It is noted that a“parking area” may also be referred to herein as a “parking space.” Toenhance the efficiency of a vehicle wireless power transfer system 100,an electric vehicle 112 may be aligned along an X direction and a Ydirection to enable an electric vehicle induction coil 116 within theelectric vehicle 112 to be adequately aligned with a base wirelesscharging system 102 a within an associated parking area.

Furthermore, the disclosed embodiments are applicable to parking lotshaving one or more parking spaces or parking areas, wherein at least oneparking space within a parking lot may comprise a base wireless chargingsystem 102 a. Guidance systems (not shown) may be used to assist avehicle operator in positioning an electric vehicle 112 in a parkingarea to align an electric vehicle induction coil 116 within the electricvehicle 112 with a base wireless charging system 102 a. Guidance systemsmay include electronic based approaches (e.g., radio positioning,direction finding principles, and/or optical, quasi-optical and/orultrasonic sensing methods) or mechanical-based approaches (e.g.,vehicle wheel guides, tracks or stops), or any combination thereof, forassisting an electric vehicle operator in positioning an electricvehicle 112 to enable an induction coil 116 within the electric vehicle112 to be adequately aligned with a charging induction coil within acharging base (e.g., base wireless charging system 102 a).

As discussed above, the electric vehicle charging system 114 may beplaced on the underside of the electric vehicle 112 for transmitting andreceiving power from a base wireless charging system 102 a. For example,an electric vehicle induction coil 116 may be integrated into thevehicles underbody preferably near a center position providing maximumsafety distance in regards to EM exposure and permitting forward andreverse parking of the electric vehicle.

FIG. 6 is a chart of a frequency spectrum showing exemplary frequenciesthat may be used for wireless charging an electric vehicle, inaccordance with an exemplary embodiment of the invention. As shown inFIG. 6, potential frequency ranges for wireless high power transfer toelectric vehicles may include: VLF in a 3 kHz to 30 kHz band, lower LFin a 30 kHz to 150 kHz band (for ISM-like applications) with someexclusions, HF 6.78 MHz (ITU-R ISM-Band 6.765-6.795 MHz), HF 13.56 MHz(ITU-R ISM-Band 13.553-13.567), and HF 27.12 MHz (ITU-R ISM-Band26.957-27.283).

FIG. 7 is a chart showing exemplary frequencies and transmissiondistances that may be useful in wireless charging electric vehicles, inaccordance with an exemplary embodiment of the invention. Some exampletransmission distances that may be useful for electric vehicle wirelesscharging are about 30 mm, about 75 mm, and about 150 mm. Some exemplaryfrequencies may be about 27 kHz in the VLF band and about 135 kHz in theLF band.

Inductive power transfer (IPT) systems provide one example of wirelesstransfer of energy. In IPT systems, a primary (or “transmitter”) powerdevice transmits power to a secondary (or “receiver”) power receiverdevice. Each of the transmitter and receiver power devices includes aninductive coupler, e.g., a single coil or a multi-coil arrangement ofwindings of electric current conveying media. An alternating current inthe primary inductor produces an alternating magnetic field. When thesecondary inductor is placed in proximity to the primary inductor, thealternating magnetic field induces an electromotive force (EMF) in thesecondary inductor (Faraday's law), thereby transferring power to thesecondary power receiver device.

A planar IPT coupler that may be also called an IPT magnetic flux devicetypically comprises a low profile planar coil structure for generatingor picking-up magnetic flux, a ferrite backing or core structure, and aconductive back plate for purposes of magnetic flux shaping andshielding. The ferrite structure may comprise ferrite tiles assembledvirtually without gaps (e.g., constituting a monolithic block) or it maycomprise ferrite slabs with gaps between the slabs with a main directionof flux parallel to the long side of the slabs. The conductive packplate can facilitate achieving the particular boundary conditionsdesired for the magnetic field in the space between ground and vehicleunderbody.

Various different planar coil coupler topologies have been proposed forinductive power transfer (IPT) from a ground-based charging unit to anelectric vehicle. These coupler topologies include, but are not limitedto: “circular”-type (e.g., single coil on top of a ferrite structure,such as a ferrite backing; see, e.g., U.S. patent application Ser. No.12/451,436, “Multi-sourced electric vehicle pick-up”); “solenoid”-type(e.g., single coil wound around a ferrite structure, such as a ferritecore; see, e.g., U.S. patent application Ser. No. 13/138,299, “Inductivepower transfer apparatus”); “double-coil”-type (e.g., two coilsessentially on top of a ferrite structure, such as a ferrite backing;see, e.g., U.S. patent application Ser. No. 13/138,298, “Inductive powertransfer apparatus”); and variants thereof (e.g., “bi-polar”-type; see,e.g., U.S. patent application Ser. No. 13/389,090, “Bi-polar paddevelopment”). In addition, other coil coupler topologies have beenproposed for IPT that are combinations of these topologies withadditional coils (e.g., U.S. patent application Ser. No. 13/791,538,“Wireless power transfer system coil arrangements and method ofoperation” which discloses an arrangement which combines a “double-D”structure with a “circular” structure).

If optimized and compared under the same size or volume constraint,these coupler topologies differ in performance characteristics such ascoupling factor, tolerance to horizontal displacement and verticaldisplacement (e.g., offset and air gap height), native quality factor,and leakage flux densities in the immediate surrounding or in thevicinity of the vehicle in case of a vehicle installation (e.g.,emissions).

Numerous computer simulations, as well as practical measurements ofdifferent coupler-type topologies and design variants have providedevidence that in certain implementations, “circular”-type coupler coilsgenerally exhibit the weakest coupling and the least tolerance but thelowest emissions and highest Q-factor of certain coupler topologiesrelative to others, while “solenoid”-type coupler coils exhibit thestrongest coupling and the largest tolerance, but the highest emissionlevels and lowest Q-factor of certain coupler topologies relative toothers. “Double-coil”- or “double-D”-type coupler coils are somewherebetween “circular”-type and “solenoid”-type coupler coils, making themparticularly interesting as a topology that exhibits design trade-offs(e.g., between coupling performance and emissions).

This aspect of “double-coil”-type coupler coils may be explained byconsidering “double coil”-type coupler topologies as a stage ofmetamorphosis between the “circular”-type and “solenoid”-typetopologies. This description of the “double-coil”-type coupler topologyas a metamorphosis of “circular”-type and “solenoid”-type couplertopologies can be helpful in understanding and explaining thecharacteristics of the various coupler topologies and to systematicallyselect (e.g., control) these characteristics and to generate new couplerdesigns that exhibit a desired trade-off between the performancecharacteristics (e.g., between coupling factor and emissions).

FIG. 8A shows a family of “double-coil”-type coupler designs whosemembers may be considered as intermediate stages of a process ofmetamorphosis of a “circular”-type coupler towards a “solenoid”-typecoupler. Particularly, these coupler designs are the so-called“bi-polar” coupler and variants of the so-called “double-D” coupler,which are of particular interest.

Two coupler topologies are of particular interest: “double-D, full-sizeferrite” coupler topology and the “double-D, front-stacked windings”coupler topology. The “double-D, full-size ferrite” coupler coil may beconsidered to be a variant of the “double-D”-type coupler coil,representing a trade-off in favor of emissions. The “double-D,front-stacked windings” coupler coil may be considered to be a variantof the “double-D”-type coupler coil, representing a trade-off in favorof coupling factor and tolerance to displacements. Using the “double-D,full-size ferrite” coupler coil in the base pad and the “double-D,front-stacked windings” coupler coil on the electric vehicle can providea good solution for a small vehicle package that integrates both couplercoils and power electronics (e.g., rectifier). The concept of the“double-D, front-stacked windings” coupler coil is also useful if both a“double-D”-type coupler coil and a “quadrature”-type coupler coil has tobe integrated into a small vehicle package with an optimum spaceutilization and good performance.

The “double-D, full-size ferrite” coupler (see, e.g., FIGS. 15A, 15B,and 25) can be a magnetic flux device 210 configured to transmit orreceive magnetic flux to or from a space beyond the magnetic flux device210. As used herein, the term “magnetic flux device” has its broadestreasonable interpretation, including but not limited to, a base pad, avehicle pad, or other type of magnetic flux pad, and is not restrictedto any particular shape, dimensions, or combination of components. Asused herein, the term “pad” has its broadest reasonable interpretation,including but not limited to, a device (e.g., a base pad, a vehicle pad)configured for use in a wireless electric vehicle charging system, andis not restricted to any particular shape, dimensions, or combination ofcomponents. The magnetic flux device 210 comprises at least a firstelectrically conductive coil 220 and a second electrically conductivecoil 230. The first coil 220 is substantially planar and has a firstperiphery bounding a first area. The second coil 230 is substantiallyplanar and has a second periphery bounding a second area. The secondcoil 230 is substantially coplanar with the first coil 220. The magneticflux device 210 further comprises a magnetically permeable material 240having a substantially planar surface 242 and having a third peripherybounding a third area. The magnetically permeable material 240 issometimes referred to herein as a “core.” As used herein, the term“core” has its broadest reasonable interpretation, which in particular,is not to limited to being in a central location or being wrapped aroundby other components. The magnetically permeable material 240 can bemagnetically associated with at least the first coil 220 and the secondcoil 230. The first coil 220 and the second coil 230 are substantiallyparallel to the substantially planar surface 242. A ratio of a sum ofthe first area and the second area to the third area is in a rangebetween 0.9 and 1.1.

The “double-D, front-stacked windings” coupler (see, e.g., FIGS. 17A and17B) can be a magnetic flux device 310 configured to transmit or receivemagnetic flux to or from a space beyond the magnetic flux device 310.The magnetic flux device 310 comprises at least a first electricallyconductive coil 320 and a second electrically conductive coil 330. Thefirst coil 320 has a first layer 322 and second layer 324. The secondcoil 330 has a third layer 332 and fourth layer 334. The first layer 322is substantially coplanar with the third layer 332. The magnetic fluxdevice 310 further comprises a magnetically permeable material 340having a substantially planar first surface 342, a second surface 343adjoined to the first surface 342 at a first edge 346, and a thirdsurface 348 adjoined to the first surface 342 at a second edge 350. Themagnetically permeable material 340 can be magnetically associated withat least the first coil 320 and the second coil 330. The first coil 320extends over the first edge 346 and intersects a plane of the firstsurface 342. The second coil 330 extends over the second edge 350 andintersects the plane of the first surface 342.

FIG. 8A shows a selection of “double-coil”-type coupler topologies forIPT which can be considered as having been generated through a processof metamorphosis that starts at the planar “circular” topology and thatends at the planar “solenoid” topology. This process of metamorphosis ingeneral is schematically displayed in FIG. 8B. In an initial step, the“circular” coil is split into a first and a second coil. Then, one coilis moved to the left and the other coil is moved to the right. Moreover,both coils are stretched to the width of the ferrite structure. Infollowing steps, coils are further stretched and pulled over the ferritestructure in a manner that the position of the inner segments (e.g.,coil segments that are adjacent) remain fixed on the upper surface ofthe ferrite and outer segments (e.g., coil segments that are on oppositeside) move to be beneath the ferrite structure, with the ferritestructure becoming a core with the coils wound around the core. In anext step, both coils are contracted in a manner that the outer coilsegments move towards the center resulting in two separate but adjacentsolenoid coils. Finally, the two solenoid coils are merged into a singlesolenoid. For reasons of comparability of performance, it can be assumedthat all the couplers as generated by metamorphosis have equal formfactors.

This process of metamorphosis is also demonstrated in a sequence ofschematic depictions starting at FIGS. 9A-9B and terminating at FIGS.23A-23B. These schematic depictions show at least a cross-section viewof the coupler structure and in some cases additionally a perspective(3D) view of the coupler. The cross-sections generally are not drawn toscale and should be considered qualitative.

FIG. 9A schematically illustrates the cross-section of a “circular”magnetic flux device (e.g., the magnetic flux device of FIG. 9B). FIG.9A also indicates the magnetic pole area (N) in the center of themagnetic flux device and the opposite pole area (S) in the peripheralzone of the magnetic flux device and two characteristic field lines. Ascompared to the other topologies of FIGS. 8A-8B, in certainconfigurations, a pair of “circular” magnetic flux devices can exhibitthe lowest coupling factor and tolerance, but the highest Q-factor andlowest emission levels (e.g., leakage flux), assuming the same size(form factor) and the same horizontal and vertical displacements for alltopologies. The low emission levels may be explained by the fact thatthe vertical magnetic field components are effectively cancelled out bythe conductive back plate (e.g., flux shaping effect) resulting in lessstray flux outside the functional space of the IPT coupling system. The“circular” coupler may therefore be considered as one extreme in thesequence of topologies shown in FIGS. 8A-8B.

FIGS. 10, 11, 12, and 13A-13B schematically illustrate steps 1, 2, 3,and 4 of a metamorphosis towards the “solenoid”: the “circular” coil issplit into coil A and coil B (see FIG. 10), coil A is moved to the left(see FIG. 11) and coil B to the right (see FIG. 12), and parts of coil Athat do not overlap with coil B are lowered (e.g., adjusted) to theplane of coil B (see FIGS. 13A-13B), resulting in a double coilstructure with overlapping coils and outer dimensions substantiallyequal to those of the ferrite structure. At a certain degree ofoverlapping, the so-called “bi-polar” magnetic flux device isencountered, characterized by virtually zero coupling between coil A andcoil B. Zero coupling (e.g., zero mutual inductance) allows coils to bedriven independently with currents of different magnitude and phase sothat the “bi-polar” coupler can be operated in a vertical, horizontal,or mixed mode of polarization. A model of an exemplary embodiment of the“bi-polar” coupler is depicted in FIG. 13B.

If coil A and coil B are driven with equal current levels and currentdirections as shown in FIG. 13A, the “bi-polar” coupler acts like a“circular” coupler generating a vertical magnetic moment as indicated bythe pole areas (N and S) and magnetic field lines in FIG. 13A. Similarlyto the “circular” coupler, it is characterized by relatively weakcoupling and displacement tolerance, but very low emission levels.

In step 5 of the metamorphosis, the current direction in coil B isreversed, as shown schematically in FIG. 14, leading to the “bi-polar”coupler operated in a horizontally polarized mode, as indicated by thetwo pole areas (N and S) and the field line. Changing current directionin one of the coils may cause certain behaviors that may be consistentwith a “solenoid”-type coupler that generates the most pronouncedhorizontal magnetic moment of the various topologies depicted in FIGS.8A-8B. Therefore, the characteristics of the “bi-polar” coupler changesubstantially. Coupling and tolerance increase, but emission levels doas well, since the conductive back plate exerts no stray fieldcancelling effect for horizontal field components. In contrast, use of aconductive back plate in the base pad and in the vehicle pad, or simplythe presence of metallic structures in the vehicle underbody and ground(e.g., ferroconcrete), may be counterproductive in regards to emissions.Conductive back plates may be used to prevent excessive eddy currentlosses (e.g., induction heating) in a vehicle's steel underbodystructure and in the steel rebar structure of a ferroconcrete ground. Onthe other hand, the use of a conductive back plate may substantiallyimprove coupling in some horizontally polarized systems (e.g.“solenoid”-type) and can partially explain the high couplingcoefficients of these coupler types as opposed to “circular”-typemagnetic flux devices where metallic structures generally exert anegative impact on coupling and performance.

FIGS. 15A-15B schematically illustrate the result of step 6 of themetamorphosis that modifies the two coils 220, 230 to becomenon-overlapping, leading to the topology termed the “double-D, full sizeferrite” coupler, which is characterized by the outer horizontaldimensions of both the coils 220, 230 and the magnetically permeablematerial 240 (e.g., ferrite structure) being substantially equal to oneanother. In certain cases, this first variant of a “double-D” couplermay exhibit the lowest emission levels among all the “double-D” variantsin the sequence as depicted in FIGS. 8A-8B, since it is ‘closest’ to the“circular”-type coupler. The “double-D, full size ferrite” topology canbe useful for a charging base as it has the potential to providesolutions generating substantially lower emissions as compared to the“solenoid” topology or other variants of the “double-D” topology.

In the example structure shown in FIGS. 15A-15B, the first coil 220 hasa first periphery (e.g., D-shaped) bounding a first area, the secondcoil 230 has a second periphery (e.g., D-shaped) bounding a second area,the magnetically permeable material 240 has a third periphery bounding athird area, and a ratio of the sum of the first area and the second areato the third area is in a range between 0.9 and 1.1. For example, thesum of the first area and the second area can be substantially equal tothe third area. One or more portions (e.g., substantially straightportions) of the first periphery can be substantially aligned with oneor more portions (e.g., substantially straight portions) of the thirdperiphery, and one or more portions (e.g., substantially straightportions) of the second periphery can be substantially aligned with oneor more portions (e.g., substantially straight portions) of the thirdperiphery. For example, an outer horizontal dimension of the sum of thefirst coil 220 and the second coil 230 (e.g., a first length across thedouble-D coils from a substantially straight portion of the firstperiphery to an opposite and substantially straight portion of thesecond periphery) can be substantially equal to an outer horizontaldimension of the magnetically permeable material 240 (e.g., a secondlength across the third periphery substantially parallel to the firstlength). Other portions of the first periphery and the second periphery(e.g., curved portions, such as the corners of the D-shaped periphery)can deviate from the third periphery, such that the sum of the firstarea and the second area can be less than the third area.

In the example structure shown in FIGS. 15A-15B, the magneticallypermeable material 240 is a monolithic ferrite plate having the thirdperiphery and the third area. In certain other configurations, themagnetically permeable material 240 can comprise multiple magneticallypermeable portions (e.g., plates, rods, blocks, tiles) which aremechanically coupled to one another to form the magnetically permeablematerial 240. These multiple magnetically permeable portions can be atleast partially spaced from one another. For example, the magneticallypermeable material 240 can comprise at least one region within the thirdarea, with the at least one region comprising a non-magnetic andnon-conductive material (e.g., air, plastic). The at least one regioncan comprise multiple regions that are adjacent to one another, multipleregions that are separate from one another (e.g., separated by a ferritematerial or an electrically conductive material), or multiple regions ofboth. The at least one region can have a summed area (e.g., sum of theareas of the at least one region) that is less than 20% of the thirdarea.

In step 7 of the metamorphosis schematically illustrated in FIGS.16A-16B, the length and width of the ferrite structure are slightlyshortened so that the planar “double-D” windings overhang the underlyingferrite structure. This topology is termed the “double-D, planaroverhanging windings” coupler and corresponds with embodiments of a“double-D” coupler. This step may be considered as a preparatory measurefor the following stages of metamorphosis where the coil windings arepulled over the ferrite. Reducing the size of the ferrite provides spacefor windings at the front faces of the ferrite under the given packageform factor constraint. Interestingly, this modification on the ferriteincreases coupling and tolerance but also emission levels relative tothe preceding “double-D” variant (e.g., as depicted in FIGS. 13A-13B).

In step 8 on the way towards the “solenoid”-type coupler, the outersegments of the first and second coils 320, 330 (e.g., the “D-coils” ofthe “double-D” coil) are pulled over the front face of the magneticallypermeable material 340 (e.g., ferrite structure). With a given magneticflux device form factor constraint and coil copper cross-section, thisstep may be performed with the planar winding structure of the initial“double-D” coupler to be deformed into a multi-layer (e.g., stacked)winding structure, leading to another “double-D” variant termed the“double-D, front stacked windings” topology, an example of which isschematically depicted in FIGS. 17A-17B. A more detailed view of anotherexample structure is provided in FIGS. 26A-26D.

This “double-D, front stacked windings” coupler can outperform the“double-D, planar overhanging windings” coupler in terms of coupling andtolerance, but can exhibit higher emission levels since it is found‘closer’ to the “solenoid”-type coupler. This step of metamorphosisenlarges the coil openings and drops coil windings (e.g., at least someof the coil windings carrying the current through the first coil 320 andthe second coil 330) below the first surface 342 of the magneticallypermeable material 340 (e.g., ferrite structure), resulting in a shiftof magnetic pole areas towards the ends of the magnetically permeablematerial 340 and hence a larger flux arch, as indicated in FIG. 17A.This modification may also increase eddy current losses as the windingsget closer to the conductive back plate.

This “double-D, front stacked windings” topology is particularlysuitable for the use on the vehicle if there is a tight volumeconstraint for the vehicle package, resulting in a solution with avehicle pad form factor considerably smaller than the base pad. A lowemission-type “double-D” topology on the ground (e.g., the “double-D,full size ferrite” magnetic flux device 210, examples of which are shownin FIGS. 15A-15B and 25) combined with a high coupling-type “double-D”coupler mounted on the vehicle (e.g., the “solenoid” or the “double-D,front stacked windings” magnetic flux device 310, an example of which isshown in FIGS. 17A and 17B) can provide a useful solution under thesecircumstances. The larger base pad can be the predominant source ofemissions and the smaller vehicle pad can be mainly responsible forcoupling and tolerance. Therefore, an approach using a topology that isemission-optimized for the base side and a topology that iscoupling-optimized for the vehicle side may be useful as an optimumtrade-off.

In the example structure shown in FIGS. 17A-17B, the first coil 320comprises at least one spiral wound coil and the second coil 330comprises at least one spiral wound coil. For example, the first coil320 can comprise a plurality of conductive windings (e.g., the firstlayer 322 and the second layer 324) and the second coil 330 can comprisea plurality of conductive windings (e.g., the third layer 332 and thefourth layer 334). In certain embodiments, the first coil 320 and thesecond coil 330 are formed by a single conductive wire wound to form thetwo coils. The first coil 320 and the second coil 330 can both beadjacent to the magnetically permeable material 340 (e.g., withoutintervening material between the first and second coils 320, 330 and themagnetically permeable material 340 as shown in FIGS. 17A-17B, or withan intervening material). The first layer 322 of the first coil 320 canextend over a first half of the first surface 342 and the third layer332 of the second coil 330 can extend over a second half of the firstsurface 342. The second layer 324 of the first coil 320 extends belowthe first surface 342 (e.g., intersects a plane of the first surface342) and the fourth layer 334 of the second coil 330 extends below thefirst surface 342 (e.g., intersects a plane of the first surface 342).In certain embodiments, neither the first coil 320 nor the second coil330 encircles the magnetically permeable material 340 (e.g., extendsfrom over the first surface 342 to below a bottom surface of themagnetically permeable material 340 opposite to the first surface 342).As shown in FIGS. 17A-17B, the first coil 320 can extend from above thefirst surface 342 to below the first surface 342 (e.g., can intersect aplane of the first surface 342) and can be adjacent to the secondsurface 343 adjoined to the first surface 342 at a first edge 346 (e.g.,extend over the first edge 346). In addition, the second coil 330 canextend from above the first surface 342 to below the first surface 342(e.g., can intersect a plane of the first surface 342) and can beadjacent to the third surface 348 adjoined to the first surface 342 at asecond edge 350 (e.g., extend over the second edge 350). In certainembodiments, the first edge 346 can be opposite to the second edge 350,as schematically shown in FIGS. 17A-17B.

In the example structure shown in FIGS. 17A-17B, the magneticallypermeable material 340 is a monolithic ferrite plate. In certain otherconfigurations, the magnetically permeable material 340 can comprisemultiple magnetically permeable portions (e.g., plates, rods, blocks,tiles) which are mechanically coupled to one another to form themagnetically permeable material 340. These multiple magneticallypermeable portions can be at least partially spaced from one another.For example, the magnetically permeable material 340 can comprise atleast one region comprising a non-magnetic and non-conductive material(e.g., air, plastic). The at least one region can comprise multipleregions that are adjacent to one another, multiple regions that areseparate from one another (e.g., separated by a ferrite material or anelectrically conductive material), or multiple regions of both. The atleast one region can have a summed area (e.g., sum of the areas of theat least one region) that is less than 20% of a total area of themagnetically permeable material 340.

In certain embodiments, the first layer 322 of the first coil 320 has afirst inner periphery bounding a first region, and the third layer 332of the second coil 330 has a second inner periphery bounding a secondregion. A first center point of the first region and a second centerpoint of the second region can be closer to the first edge 346 and thesecond edge 350, respectively, than to a center point of themagnetically permeable material 340. In certain embodiments, a firstgeometric plane defined by at least one turn of each of the first coil320 and the second coil 330 in the first layer 322 and the third layer332, respectively, is parallel to the substantially planar first surface342.

FIGS. 26A-26C shows a transparent top-down view, a perspective cut view,and an explosion view, respectively, of a model of the “double-D, frontstacked windings” coupler magnetic flux device 310 in accordance withcertain embodiments described herein. By virtue of the first coil 320extending over the first edge 346 and intersecting a plane of the firstsurface 342 and the second coil 330 extending over the second edge 350and intersecting the plane of the first surface 342, certain embodimentsdescribed herein provide a potential space for electronics in a smallvehicle package integrated solution using a “double-D, front stackedwinding” coupler magnetic flux device 310. A bottom-view of an exampleof such a magnetic flux device 310 is shown schematically by FIG. 26D.The magnetic flux device 310 comprises one or more regions 360 boundedat least in part by the first coil 320, the second coil 330, and themagnetically permeable material 340. The one or more regions 360 of FIG.26D are positioned on opposite sides of the magnetically permeablematerial 340 below the undersides of the first coil 320 and the secondcoil 330. These regions can be configured to contain electroniccomponents (e.g., power conversion electronics and sensor electronics ofthe magnetic flux device 310).

Continuing the metamorphosis of the “double-D” with steps 9 and 10, theouter segments of the “double-D” windings can be completely pulled overthe front faces of the ferrite and the ferrite can be lifted up, makingroom for windings below the ferrite. The resulting new topology,depicted in FIG. 18, can be considered a variant of a “solenoid”-typecoupler since the coils are wound around a ferrite core. However, thetwo coils are very oblique and are still with front stacked windings,which is termed the “double solenoid, front stacked windings” topology.This step may also include reducing the thickness of the coils and/orthe ferrite structure if the overall height of the magnetic flux deviceis to be maintained (not shown in FIG. 18). Additionally, the outerwindings segments can now be very close to the back plate and may have anegative impact on the Q-factor of the coils. On the other hand,coupling may be substantially increased, partially compensating for theloss in Q-factor and still resulting in an acceptable efficiency.

In the following steps (step 11, 12, 13, and 14), the two solenoid coilsare successively contracted (e.g., shrunk), keeping the center segments(above ferrite) fixed so that the coil segments below the ferrite aremoving step by step towards the center of the magnetic flux device. Thisprocess of metamorphosis can generate some variants of “double solenoid”topologies and finally end up in the “solenoid” topology. In step 10,the bottom coil segment is unfolded (e.g., all windings in a singleplane), resulting in a variant that is schematically depicted in FIGS.19A-19D and termed “double solenoid, oblique windings”. In step 11, thelength of the ferrite is increased to its ‘full size’ resulting in atopology termed “double solenoid, oblique windings, full size ferrite,”as schematically depicted in FIGS. 20A-20C. This topology may beconsidered in analogy to the “double-D, full size ferrite” coupler (see,e.g., FIGS. 15A-15B and 25). In steps 12 and 13, the coils are furthercontracted, leading first to the “double solenoid, slightly oblique”coupler (see, e.g., FIGS. 20A-20C) and then to the “double solenoid,coils adjacent” coupler. Finally, in step 14, the two coils are mergedinto a single “solenoid” topology, the topology that provides thestrongest coupling but also the highest emission levels among all thetopologies shown in FIGS. 8A-8B.

In certain embodiments, a further advantage of a “double-D front stackedwindings” configuration with a reduced ferrite structure and stackedwindings (e.g., examples of which is schematically illustrated by FIGS.17A-17B and FIGS. 26A-26D) may be found when designing a so-calledcross-polar coupler (referred to as a “DDQ” coil arrangement) thatintegrates both a “double-D” (DD) coil and a “circular” coil, referredto herein as a “quadrature” (Q) coil, such that the “DDQ” coil is ableto pick-up both vertical and horizontal flux components. The cross-polarcoupler has the potential of providing more displacement tolerance inboth the x and y direction at the same time. This concept may also applyto the base (e.g., primary) side. In addition, as described more fullybelow, the cross-polar coupler or “DDQ” coil arrangement may be usefulto exploit the available space to the maximum extent possible (e.g., byleaving only a minimum air space open).

FIGS. 27A-27C schematically illustrate an example magnetic flux device410 (e.g., a cross-polar coupler or “DDQ” coil arrangement) forwirelessly receiving or transmitting power from or to a space beyond themagnetic flux device 410. The magnetic flux device 410 comprises a firstconductive structure 420 (e.g., a “DD-coil”) configured to wirelesslyreceive or transmit power via a magnetic field. The first conductivestructure 420 comprises a first coil 422 (e.g., a first D-coil) having afirst lower surface and a second coil 424 (e.g., a second D-coil) havinga second lower surface. The first lower surface of the first coil 422 issubstantially coplanar with the second lower surface of the second coil424. The first conductive structure 420 has a first length (L₁) and afirst width (W₁) that are both substantially parallel to the first andsecond lower surfaces, and the first length is greater than the firstwidth. The magnetic flux device 410 further comprises a secondconductive structure 430 (e.g., a Q-coil) configured to wirelesslyreceive or transmit power via the magnetic field. The second conductivestructure 430 has a second length (L₂) and a second width (W₂) bothsubstantially parallel to the first and second lower surfaces, and thesecond length is substantially parallel to the first length and isgreater than the second width. At least a first planar portion 426 ofthe first conductive structure 420 is substantially coplanar with asecond planar portion 436 of the second conductive structure 430.

In certain embodiments, the first conductive structure 420 comprises afirst layer of one or more conductive windings defining a firstgeometric plane that is parallel to and in a different layer than asubstantially planar surface of the second conductive structure 430 andthe first conductive structure 420 further comprises a second layer ofone or more conductive windings defining a second geometric plane thatat least partially intersects (e.g., is coplanar with) a third geometricplane defined by the substantially planar surface. The first conductivestructure 420 can have a first inner periphery bounding a first region,and the second conductive structure 430 can have a second innerperiphery bounding a second region, wherein one or more conductivewindings of the second conductive structure 430 are positioned withinthe first and second regions and are substantially coplanar with thefirst layer and positioned in a different layer than the second layer.

In certain embodiments, as schematically shown in FIGS. 27A and 27C, thefirst conductive structure 420 (e.g., the first coil 422 and the secondcoil 424) and the second conductive structure 430 are configured tosubstantially completely cover a substantially planar surface 442 of themagnetically permeable material 440. In certain embodiments, asschematically shown in FIGS. 27A-27C, the first conductive structure 420and the second conductive structure 430 are stacked on one another. Ascan be seen in FIG. 27C, the first planar portion 426 of the firstconductive structure 420 at least partially bounds at least one regioncontaining the second planar portion 436 of the second conductivestructure 430. In certain such embodiments, the magnetic flux device 410advantageously provides an optimum space utilization by exploiting theavailable space to the maximum extent possible (e.g., by leaving only aminimum air space open).

In certain embodiments, as schematically shown in FIG. 27A, the firstlength is greater than the second length, and the first width issubstantially equal to the second width. In certain embodiments, thefirst coil 422 and the second coil 424 enclose a first area and a secondarea, respectively, and the second conductive structure 430 encloses athird area. The first conductive structure 420 can have a first edge anda second edge each intersecting a first geometric line running along thefirst length of the first conductive structure 420. In certainembodiments, the first geometric line runs along the second length ofthe second conductive structure 430 as well, while in certain otherembodiments, the first geometric line is substantially parallel to asecond geometric line which runs along the second length of the secondconductive structure 430. In certain embodiments, the magnetic fluxdevice 410 comprises one or more regions bounded at least in part by thefirst conductive structure 420, the second conductive structure 430, andthe magnetically permeable material 440. The one or more regions can bepositioned on opposite sides of the magnetically permeable material 440below the undersides of the first conductive structure 420 and thesecond conductive structure 430. These regions can be configured tocontain electronic components (e.g., power conversion electronics andsensor electronics of the magnetic flux device 410).

To accommodate a “DDQ” coil arrangement (e.g., as schematicallyillustrated in FIGS. 27A-27C), it can be useful to exploit the availablespace to the maximum extent possible (e.g., by leaving only a minimumair space open). Optimum utilization of the available space for ferriteand copper (e.g., Litz wire) may be particularly useful for tight formfactor constraints (e.g., for the vehicle package). Therefore, fillingthe space at the front faces of the ferrite with stacked windings can bea useful approach with a positive effect in regards to both coupling andspace utilization. It can provide enough room for embedding the ‘Q’ coilin the openings of the ‘DD’ coil, and in the same plane directly on topof the ferrite structure, as shown in the perspective cut view of FIG.27C. This approach can be useful for a low profile magnetic flux devicesolution. Due to the reduced size ferrite, there can also be some spaceon each side of the magnetic flux device to accommodate the sidesegments of the ‘DD’ and ‘Q’ coil windings which are on top of eachother. An optimum utilization of the space at the side of the ferritemay be achieved with a staggered and stacked coil windings, as can beseen in FIG. 27B.

The various operations of methods described above may be performed byany suitable means capable of performing the operations, such as varioushardware and/or software component(s), circuits, and/or module(s).Generally, any operations illustrated in the Figures may be performed bycorresponding functional means capable of performing the operations.

Information and signals may be represented using any of a variety ofdifferent technologies and techniques. For example, data, instructions,commands, information, signals, bits, symbols, and chips that may bereferenced throughout the above description may be represented byvoltages, currents, electromagnetic waves, magnetic fields or particles,optical fields or particles, or any combination thereof.

The various illustrative logical blocks, modules, circuits, andalgorithm steps described in connection with the embodiments disclosedherein may be implemented as electronic hardware, computer software, orcombinations of both. To clearly illustrate this interchangeability ofhardware and software, various illustrative components, blocks, modules,circuits, and steps have been described above generally in terms oftheir functionality. Whether such functionality is implemented ashardware or software depends upon the particular application and designconstraints imposed on the overall system. The described functionalitymay be implemented in varying ways for each particular application, butsuch implementation decisions should not be interpreted as causing adeparture from the scope of the embodiments of the invention.

The various illustrative blocks, modules, and circuits described inconnection with the embodiments disclosed herein may be implemented orperformed with a general purpose processor, a Digital Signal Processor(DSP), an Application Specific Integrated Circuit (ASIC), a FieldProgrammable Gate Array (FPGA) or other programmable logic device,discrete gate or transistor logic, discrete hardware components, or anycombination thereof designed to perform the functions described herein.A general purpose processor may be a microprocessor, but in thealternative, the processor may be any conventional processor,controller, microcontroller, or state machine. A processor may also beimplemented as a combination of computing devices, e.g., a combinationof a DSP and a microprocessor, a plurality of microprocessors, one ormore microprocessors in conjunction with a DSP core, or any other suchconfiguration.

The steps of a method or algorithm and functions described in connectionwith the embodiments disclosed herein may be embodied directly inhardware, in a software module executed by a processor, or in acombination of the two. If implemented in software, the functions may bestored on or transmitted over as one or more instructions or code on atangible, non-transitory computer-readable medium. A software module mayreside in Random Access Memory (RAM), flash memory, Read Only Memory(ROM), Electrically Programmable ROM (EPROM), Electrically ErasableProgrammable ROM (EEPROM), registers, hard disk, a removable disk, a CDROM, or any other form of storage medium known in the art. A storagemedium is coupled to the processor such that the processor can readinformation from, and write information to, the storage medium. In thealternative, the storage medium may be integral to the processor. Diskand disc, as used herein, includes compact disc (CD), laser disc,optical disc, digital versatile disc (DVD), floppy disk and blu ray discwhere disks usually reproduce data magnetically, while discs reproducedata optically with lasers. Combinations of the above should also beincluded within the scope of computer readable media. The processor andthe storage medium may reside in an ASIC. The ASIC may reside in a userterminal. In the alternative, the processor and the storage medium mayreside as discrete components in a user terminal.

For purposes of summarizing the disclosure, certain aspects, advantagesand novel features of the inventions have been described herein. It isto be understood that not necessarily all such advantages may beachieved in accordance with any particular embodiment of the invention.Thus, the invention may be embodied or carried out in a manner thatachieves or optimizes one advantage or group of advantages as taughtherein without necessarily achieving other advantages as may be taughtor suggested herein.

Various modifications of the above described embodiments will be readilyapparent, and the generic principles defined herein may be applied toother embodiments without departing from the spirit or scope of theinvention. Thus, the present invention is not intended to be limited tothe embodiments shown herein but is to be accorded the widest scopeconsistent with the principles and novel features disclosed herein.

What is claimed is:
 1. A magnetic flux device for wireless powertransfer configured to transmit or receive magnetic flux to or from aspace beyond the magnetic flux device, the magnetic flux devicecomprising: at least a first electrically conductive coil and a secondelectrically conductive coil, the first coil having a first section anda second section and the second coil having a third section and a fourthsection, the first section substantially coplanar with the third sectionand the second section substantially coplanar with the fourth section; amagnetically permeable material having: a first side having a firstlength, a first width and a first center, and a second side,substantially parallel to the first side, having a second length, asecond width, and a second center; and an electrically conductivematerial having a first side substantially parallel to the second sideof the magnetically permeable material; the first section and the thirdsection disposed on the first side of the magnetically permeablematerial, the second section and the fourth section disposed on thesecond side of the magnetically permeable material between themagnetically permeable material and the electrically conductivematerial, the first section and the third section positioned closer tothe first center than the second section and the fourth section arepositioned to the second center, the first section and the secondsection non-overlapping and connected to bound a first region, the thirdsection and the fourth section non-overlapping and connected to bound asecond region substantially coplanar with the first region, the firstsection positioned closer to the third section than to the secondsection, and the third section positioned closer to the first sectionthan to the fourth section.
 2. The magnetic flux device of claim 1,wherein the first coil comprises at least one spiral wound coil and thesecond coil comprises at least one spiral wound coil.
 3. The magneticflux device of claim 1, wherein the first side is opposite to the secondside.
 4. The magnetic flux device of claim 1, wherein the first sectionis adjacent to the third section on the first side and the secondsection is spaced apart from the fourth section on the second side. 5.The magnetic flux device of claim 1, wherein the magnetically permeablematerial comprises a ferrite plate.
 6. The magnetic flux device of claim1, wherein the first section and the second section comprise stackedwindings of the first coil and the third section and the fourth sectioncomprise stacked windings of the second coil.
 7. The magnetic fluxdevice of claim 1, wherein the first section and the second sectioncomprise a plurality of layers of conductive windings.
 8. The magneticflux device of claim 1, wherein the first coil and the second coil forma first conductive structure having at least a first planar portion, themagnetic flux device further comprising a second conductive structureconfigured to wirelessly receive or transmit power via the magneticfield, the second conductive structure having at least a second planarportion substantially coplanar with the first planar portion.
 9. Themagnetic flux device of claim 8, wherein the first conductive structureand the second conductive structure are collectively configured to coverat least a portion of the first side of the magnetically permeablematerial.
 10. The magnetic flux device of claim 8, wherein the firstconductive structure, the second conductive structure, and themagnetically permeable material at least partially bound a regionconfigured to contain electronic components.
 11. The magnetic fluxdevice of claim 8, wherein the first conductive structure and the secondconductive structure are stacked on one another.
 12. The magnetic fluxdevice of claim 1, wherein a distance between an outer edge of thesecond section and an outer edge of the fourth section is substantiallyequal to a length of the first and second sides of the magneticallypermeable material.
 13. The magnetic flux device of claim 1, wherein adistance between an outer edge of the second section and an outer edgeof the fourth section is less than a length of the first and secondsides of the magnetically permeable material.
 14. The magnetic fluxdevice of claim 1, wherein the first section and the second section areconnected as a continuous winding to form the first coil and the thirdsection and the fourth section are connected as a continuous winding toform the second coil, wherein the coils are oblique with respect to eachother and wherein both coils are oblique to the magnetically permeablematerial.
 15. The magnetic flux device of claim 1, wherein two differentmagnetic pole areas are defined in the first region and the secondregion respectfully.
 16. The magnetic flux device of claim 1, wherein aplane defined by the magnetically permeable material along the firstlength and first width is substantially coplanar with the first regionand the second region.
 17. The magnetic flux device of claim 1, whereinthe second section is positioned closer to a first outer edge of themagnetic permeable material than to the first section, and wherein thefourth section is positioned closer to a second outer edge of themagnetic permeable material than to the third section.
 18. A magneticflux device for wireless power transfer configured to transmit orreceive magnetic flux to or from a space beyond the magnetic fluxdevice, the magnetic flux device comprising: at least a firstelectrically conductive coil and a second electrically conductive coil,the first coil having a first section and a second section connected asa continuous winding to form the first coil, and the second coil havinga third section and a fourth section connected as a continuous windingto form the second coil, the first section substantially coplanar withthe third section and the second section substantially coplanar with thefourth section; a magnetically permeable material having: a first side,and a second side substantially opposite the first side; and anelectrically conductive material having a first side substantiallyparallel to the second side of the magnetically permeable material, thefirst section and the third section disposed on the first side, thesecond section and the fourth section disposed on the second sidebetween the magnetically permeable material and the electricallyconductive material, and wherein a plane of the first coil formed bybisecting the first section and second section is disposed in an obliquearrangement relative to the first and second side of the magneticallypermeable material and wherein a plane of the second coil formed bybisecting the third section and fourth section is disposed in an obliquearrangement relative to the first and second side of the magneticallypermeable material, the first section and the second sectionnon-overlapping, the third section and the fourth sectionnon-overlapping, the first section positioned closer to the thirdsection than to the second section, and the third section positionedcloser to the first section than to the fourth section.
 19. A magneticflux device for wireless power transfer configured to transmit orreceive magnetic flux to or from a space beyond the magnetic fluxdevice, the magnetic flux device comprising: a first electricallyconductive coil and a second different electrically conductive coil, thefirst coil having a first section and a second section and the secondcoil having a third section and a fourth section, the first sectionsubstantially coplanar with the third section and the second sectionsubstantially coplanar with the fourth section; means for modifyingmagnetic flux generated by the first electrically conductive coil andthe second different electrically conductive coil, the modifying meanshaving: a first side having a first length, a first width, and a firstcenter, and a second side, substantially parallel with the first side,having a second length, a second width, and a second center; and anelectrically conducting means having a first side substantially parallelto the second side of the modifying means, the first section and thethird section disposed on the first side of the modifying means, thesecond section and the fourth section disposed on the second side of themodifying means between the modifying means and the electricallyconducting means, and the first section and the third section positionedcloser to the first center than the second section and the fourthsection are positioned to the second center, the first section and thesecond section non-overlapping and connected to bound a first region,the third section and the fourth section non-overlapping and connectedto bound a second region substantially coplanar with the first region,the first section positioned closer to the third section than to thesecond section, and the third section positioned closer to the firstsection than to the fourth section.